Download Advances in Electronics and Electron Phisics. Vol. 43 by Ladislaus Marton PDF

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D. , and Millward, G. R. (1970). J. Ultrastruct. Res. 31, 203. Garrod, R. , and Nankivell, J. F. (1958). Brit. J. Appl. Phys. 9, 214. Glick, A. J. (1965). In “Qualitative Electron Microscopy” (G. F. Bahr and E. M. ), p. 49. Williams & Wilkins, Baltimore, Maryland. Goldfischer, L. I. (1965). J . Opt. Am. 55, 247. Hall, C. E. (1953). ” McGraw-Hill, New York. Hanszen, K. J. (197 1). Adu. Opt. Electron Microsc. 4, 1. Hanszen, K. J. (1973). In “Image Processing and Computer-aided Design in Electron Optics” (P.

1971). Phil. Trans. R. London, Ser. B 261, 71. Horne, R. W, and Markham, R. (1972). I n “Practical Methods in Electron Microscopy” (A. M. ), vol. 1, Part 11, p. 327. , Amsterdam. Johansen, B. V. (1973). Micron 4, 446. Klug, A. (1971). Phil. Trans. R. London, Ser. B 261, 173. Klug, A,, and Berger, J. E. (1964). J . Mol. Biol. 10, 565. , and De Rosier, D. J. (1966). Nature (London)212, 29. , Crick, F. H. , and Wyckoff, H. W. (1958). Acta Crystallogr. 11, 199. Lake, J. A. (1972). I n “Optical Transforms” (H.

T(v) ~ ( v ) ] (105) In the case of a point object, the restoration of the image thus performed optimizes the contrast (Lenz, 1970). In effect the spectrum of a point object is a constant, A(v) = c 0 , and its reconstructed image after zonal filtering, from Eq. (126), is given by ci(r) = e0 * r ' [ H ( v )* T ( v ) ] (106) + The contrast at the center of the image is then simply Cl(0) = const. x ( H ( v ) . T ( v ) ) (107) taking into account that the Fourier transform in the origin is proportional to the mean value of the function on which it operates.

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